Panel 1. See full resolution. The second spectrum line from the right is a flaw. The iconic 4686 line of ionized helium (He II) to the right of center is very strong, as are the forbidden triply-ionized [Ar IV] lines. |
Panel 2. See full resolution . The spectrum is dominated by the H-Gamma line at 4340 Angstroms toward the left. The [O III] line from doubly ionized oxygen at 4363 Angstroms is used along with those at 4959 and 5007 Angstroms (the "nebulium" lines: see IC 418 and the Ring Nebula) to measure nebular temperatures. Just to the left of it at 4358 Angstroms is a line from Los Angeles street lights (this and others giving mercury vapor lamps their blue color.) The strong neutral helium (He I) line at 4471 Angstroms to the right, along with the 4686 Angstrom He II line seen in Panel 1, is used to measure nebular helium compositions. |
Panel 3. See full resolution. The spectrum is dominated by the H-Delta line at 4101 Angstroms toward far left. To the right, at a wavelength of 4267 Angstroms, is an important line of ionized carbon (C II) used to get nebular carbon compositions. |
Panel 4. See full resolution. Three more hydrogen lines, H-Epsilon (or H7) at 3970 Angstroms, H8 at 3889, and H9 at 3835 show the hydrogen spectrum beginning to pile up toward the limit at 3646 Angstroms as seen in the next panel. The forbidden doubly ionized neon [Ne III] line to the left of center at 3868 Angstroms is crucial for obtaining neon compositions. It is coupled to the 3967 line at center that is usually blended with the hydrogen and helium lines to either side of it. Note the highly ionized iron line at 3895 Angstroms. |
Panel 5. See full resolution. We arrive at the dramatic confluence of the Balmer lines and the beginning of the Balmer continuum, which stretches out to the left. It's marred somewhat by a couple strong lines from Los Angeles. The critical forbidden ionized oxygen lines at 3726 and 3728, used to derive nebular densities (and together nebular oxygen compositions), are well separated. At lower resolution they are often blended into one. |
Panel 6. See full resolution. The Balmer continuum weakens toward shorter wavelengths; note the strong O III lines from doubly-ionized oxygen. They are pumped up to higher intensities by a fluorescent mechanism. Numerous neutral helium lines, which are cascading toward their own limit, fall to the right of center. |
Panel 7. See full resolution. The 3203 line of He II, coupled to the 4686 He II line in Panel 1, is also strong as is the last of the observed O III lines. Beyond this point little radiation penetrates the Earth's atmosphere, compliments mostly of ozone. |